Info  

14.04.17 Racing starts today at 12:00  
13.04.17 Racing postponed for tommorow 
Nicholas Estep
@NicholasEstep

25 Aug 14  
вЂњ@Deadspin: The footwork in this Vine from Saints DB drills is mesmerizing: deadsp.in/4jUjsF7вЂќ


Authors  Formulations 

Price, 1984 [8]  T_{s} = a_{0} + a_{1}T_{i} + a_{2}(T_{i} − T_{j}) + a_{3}(T_{i} − T_{j})(1 − ε) + a_{4}T_{j}Δε 
Prata and Platt, 1991 [14]  ${T}_{s}={a}_{0}+{a}_{1}\frac{{T}_{i}}{\mathit{\epsilon}}+{a}_{2}\frac{{T}_{j}}{\mathit{\epsilon}}+{a}_{3}\frac{1\mathit{\epsilon}}{\mathit{\epsilon}}$ 
Vidal, 1991 [15]  ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}{T}_{j})+{a}_{3}\frac{1\mathit{\epsilon}}{\mathit{\epsilon}}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ 
Ulivieri et al., 1992 [16]  T_{s} = a_{0} + a_{1}T_{i} + a_{2}(T_{i} − T_{j}) + a_{3}(1 − ε) + a_{4}Δε 
Sobrino et al., 1993 [17]  T_{s} = a_{0} + a_{1}T_{i} + a_{2}(T_{i} − T_{j}) + a_{3}(T_{i} − T_{j})^{2} + a_{4}(1 − ε) + a_{5}Δε 
Sobrino et al., 1994 [18]  ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}{T}_{j})+{a}_{3}\mathit{\epsilon}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ 
Coll et al., 1997 [19]  T_{s} = T_{i}+ a_{0} + a_{1}(T_{i} − T_{j}) + a_{2}(T_{i} − T_{j})^{2} + a_{3}(1 − ε) + a_{4}Δε 
Authors  Formulations 

Price, 1984 [8]  T_{s} = a_{0} + a_{1}T_{i} + a_{2}(T_{i} − T_{j}) + a_{3}(T_{i} − T_{j})(1 − ε) + a_{4}T_{j}Δε 
Prata and Platt, 1991 [14]  ${T}_{s}={a}_{0}+{a}_{1}\frac{{T}_{i}}{\mathit{\epsilon}}+{a}_{2}\frac{{T}_{j}}{\mathit{\epsilon}}+{a}_{3}\frac{1\mathit{\epsilon}}{\mathit{\epsilon}}$ 
Vidal, 1991 [15]  ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}{T}_{j})+{a}_{3}\frac{1\mathit{\epsilon}}{\mathit{\epsilon}}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ 
Ulivieri et al., 1992 [16]  T_{s} = a_{0} + a_{1}T_{i} + a_{2}(T_{i} − T_{j}) + a_{3}(1 − ε) + a_{4}Δε 
Sobrino et al., 1993 [17]  T_{s} = a_{0} + a_{1}T_{i} + a_{2}(T_{i} − T_{j}) + a_{3}(T_{i} − T_{j})^{2} + a_{4}(1 − ε) + a_{5}Δε 
Sobrino et al., 1994 [18]  ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}{T}_{j})+{a}_{3}\mathit{\epsilon}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ 
Coll et al., 1997 [19]  T_{s} = T_{i}+ a_{0} + a_{1}(T_{i} − T_{j}) + a_{2}(T_{i} − T_{j})^{2} + a_{3}(1 − ε) + a_{4}Δε 
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